US3089034A - Light sensitive detection circuit - Google Patents
Light sensitive detection circuit Download PDFInfo
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- US3089034A US3089034A US53020A US5302060A US3089034A US 3089034 A US3089034 A US 3089034A US 53020 A US53020 A US 53020A US 5302060 A US5302060 A US 5302060A US 3089034 A US3089034 A US 3089034A
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- 238000011896 sensitive detection Methods 0.000 title description 6
- 238000001514 detection method Methods 0.000 claims description 19
- 230000001172 regenerating effect Effects 0.000 claims description 14
- 230000005540 biological transmission Effects 0.000 claims description 4
- 230000010355 oscillation Effects 0.000 description 7
- 239000003990 capacitor Substances 0.000 description 6
- 230000008859 change Effects 0.000 description 4
- 230000007423 decrease Effects 0.000 description 4
- 230000010363 phase shift Effects 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 229940056932 lead sulfide Drugs 0.000 description 1
- 229910052981 lead sulfide Inorganic materials 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 238000005057 refrigeration Methods 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/10—Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors
- G01J5/28—Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors using photoemissive or photovoltaic cells
- G01J5/30—Electrical features thereof
Definitions
- the present invention relates to a temperature responsive detection device and in particular to such a device having a regenerative feedback circuit which drives an amplifier into oscillation when the sensed temperature exceeds a predetermined value.
- the resistance of infra-red detector cells of the lead sulfide type varies inversely with cell temperature and inversely with infra-red energy.
- the change of resistance of the cell as a result of infra-red energy change is small as compared to the change of cell resistance as a result of the change of cell temperature.
- the response characteristic of an infra-red cell, responsive to and operating in long infra-red wave length regions is at an optimum at very low temperatures. Therefore, in order to successfully operate an infra-red detector cell of this type, it is necessary to maintain the cell at a very low constant temperature. Cooling devices which are not subject to manual control, in missiles for example, are seldom completely reliable and it is necessary that a temperature detector be provided in order to determine whether or not operation is permissible.
- Prior temperature responsive detection devices have included micro-ammeter detection circuits. However, since the currents to be detected are extremely small, the accuracy and reliability of equipment of this type is not satisfactory. Furthermore, additional lead lines from the missile, for example, are necessary in order to provide the required information.
- the present invention overcomes the aforementioned difficulties by utilizing existing and conventional circuitry (power supply, amplifier stages, frequency detector, etc.) and incorporating a diode-controlled regenerative feedback circuit to drive the amplifier into oscillation when the temperature of the infra-red detector cell increases to a predetermined value.
- the tone detected by the frequency detector an earphone, for example
- the amplifier is in oscillation is readily distinguishable from the tone produced by the normal cell output signal thereby providing information for the operator as to whether or not operation is permissible.
- An object of the present invention is to provide a simple, inexpensive temperature detection device.
- Another object is to sense a predetermined temperature of an infra-red sensitive detection cell.
- Still another object is to oscillate the amplifier of an infra-red sensitive detection cell when the temperature of the cell exceeds a predetermined value.
- Still another object is to oscillate the amplifier of an infra-red sensitive detection cell by means of a regenerative feedback which is operative when the temperature of the cell exceeds a predetermined value.
- Still another object is to oscillate an amplifier by means of a regenerative feedback when the input voltage is at a predetermined value.
- the FIGURE is a schematic diagram of the present invention.
- detector cell 11 which is responsive to long wave length infra-red radiation.
- cells of this type must be maintained at very low temperatures, l96 C. for example, by means of separate refrigeration equipment shown by broken lines and designated generally by numeral 12.
- a detector cell of this type has a large negative temperature coelficient and when cooled to its operating temperature, 196 C. for example, its resistance will be approximately 3,500K ohms and when at room temperature its resistance will be approximately 50K ohms.
- the cell bias circuit consists of decoupling resistor 13 and cell load resistor 15 which series connect cell 11 with a B+ D.C. power supply.
- Capacitor 17 is provided to filter A.C. components from the DC. B+ power supply. It should be noted that the voltage at E between resistors 13 and 15, will decrease with increased detector cell temperature since the resistance of the detector cell decreases with increased temperature.
- An R-C amplifier circuit is provided which is conventional and consists of triodes 21, '22 and 23 which are plate biased by B+ power through resistors 24, 25 and 26, respectively, and grid biased through resistors 27, 28 and 29, respectively.
- the output of cell 11 is coupled to the grid of triode 21 through coupling capacitor 31 and triodes 22 and 23 are coupled by capacitors 33 and 35, respectively.
- the triode 23 is of the cathode follower type, the cathode thereof being connected through resistor 37 to ground.
- the feedback circuit is regenerative and connects the cathode of triode 23 to the grid of triode 2.1 through D.-C. blocking capacitor 38, diode 39, resistor 15 and capacitor 31. It can be seen that the feedback is regenerative since the phase shift from the grid of triode 21 to the grid of cathode follower triode 23 is 360 and since the cathode voltage follows the grid voltage of triode 23, the cathode of triode 23 has a 360' phase shift from the grid of triode 21.
- the cathode of diode 39 is biased by the voltage at B
- a voltage dividing network designated generally by numeral 41 provides a voltage E between resistors 42 and 43.
- the anode of diode 39 is biased by the voltage at E through current limiting resistor 44.
- Diode 39 which may be of the silicon type, is used as a switch and provides infinite resistance when it is non-conducting. Diode 39 is non-conducting when E E and is conducting when E E.
- the gain of the three stage amplifier is such that the amplifier will oscillate, at a frequency determined by the amplifier characteristics, when the regenerative feedback signal is applied to the input thereof. Voltage gain of the amplifier is sufiicient to cause oscillation even though the feedback is not connected directly to the grid but Reference Numeral Unit Value
- the operation of the device is as follows: When the cell is at its normal operating temperature (-196" C.) the voltage at E is approximately 155 volts.
- diode 39 Since E is approximately 134 volts, diode 39 is reverse biased and provides infinite resistance. Therefore, the feedback from triode 23 is not applied to the grid of triode 21 and the amplifier functions as an amplifier of the signal from cell 11. As the temperature of cell 11 increases, the voltage at E decreases. Diode 39 will conduct when E decreases to a value less than E since it. is then forward biased. When diode 39 conducts, a regenerative feedback signal from the cathode of triode 2.3 is applied to the grid of triode 21 which causes the amplifier to oscillate at its natural frequency. The output of the amplifier is applied to a frequency responsive device, earphones for example, which indicates whether the amplifier is oscillating or is normally amplifying the cell output signal.
- a detection device comprising an amplifier, a detection cell responsive to light energy, the resistance of said detection cell varying inversely with the temperature of said cell, a resistor, one side of said resistor being connected to a DC. potential source, the other side of said resistor being connected to one side of said detection cell, the other side of said detection cell being connected to ground, said one side of said detection cell being connected to the input of said amplifier, a regenerative feedback network for interconnecting the output and input of said amplifier, and means responsive to the voltage at said other side of said resistor for controlling transmission of the amplifier output signal through said network, wherein said last mentioned means comprises a diode the cathode of which is connected to said other side of said resistor and the anode of which is connected to a fixed D.C.
- a detection device comprising an amplifier, a detection cell responsive to infra-red energy, the resistance of said detection cell varying inversely with the temperature of said cell, first and second resistors and said cell respectively connected in series with a DC.
- a regenerative feedback circuit comprising a diode, the cathode of said diode being connected between said first and second resistors and the anode of said diode being connected to the output of said amplifier and to a DC. potential source, the DC. voltage at said anode being less than the DC. voltage at said cathode when said cell is at a temperature not greater than a predetermined value, thereby preventing the transmission of the regenerative amplifier output signal to said input, and the DC. voltage at said anode being greater than the DJC. voltage at said cathode when the cell is at a temperature greater than said predetermined value, thereby permitting transmission of said regenerative output signal to said input and thereby causing said amplifier to oscillate.
- a frequency detection device is connected to the output of said amplifier for detecting whether the amplifier is oscillating.
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Description
y 7, 1963 R. c. MEADE 3,089,034
LIGHT SENSITIVE DETECTION CIRCUIT Filed Aug. 30, 1960 3 If 2 o u 2 w m u I g o m E :2
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- 3 EL N 5 1- E P w E r 2 3 4 E LU 2 a w m EBP W I}. m
I I INVENTOR.
ROBERT C. MEADE Evy/d cAMA 251 a ATTORNEYS.
United States Patent 3,089,034 LIGHT SENSITIVE DETECTION CIRCUIT Robert C. Meade, China Lake, Califi, assignor to the United States of America as represented by the Secretary of the Navy Filed Aug. 30, 1960, Ser. No. 53,020 3 Claims. (Cl. 250-214) (Granted under Title 35, US. Code (1952), sec. 266) The invention herein described may be manufactured and used by or for the Government of the United States of America for governmental purposes without the payment of any royalties thereon or therefor.
The present invention relates to a temperature responsive detection device and in particular to such a device having a regenerative feedback circuit which drives an amplifier into oscillation when the sensed temperature exceeds a predetermined value.
The resistance of infra-red detector cells of the lead sulfide type, for example, varies inversely with cell temperature and inversely with infra-red energy. The change of resistance of the cell as a result of infra-red energy change is small as compared to the change of cell resistance as a result of the change of cell temperature. In addition, the response characteristic of an infra-red cell, responsive to and operating in long infra-red wave length regions, is at an optimum at very low temperatures. Therefore, in order to successfully operate an infra-red detector cell of this type, it is necessary to maintain the cell at a very low constant temperature. Cooling devices which are not subject to manual control, in missiles for example, are seldom completely reliable and it is necessary that a temperature detector be provided in order to determine whether or not operation is permissible.
Prior temperature responsive detection devices have included micro-ammeter detection circuits. However, since the currents to be detected are extremely small, the accuracy and reliability of equipment of this type is not satisfactory. Furthermore, additional lead lines from the missile, for example, are necessary in order to provide the required information.
The present invention overcomes the aforementioned difficulties by utilizing existing and conventional circuitry (power supply, amplifier stages, frequency detector, etc.) and incorporating a diode-controlled regenerative feedback circuit to drive the amplifier into oscillation when the temperature of the infra-red detector cell increases to a predetermined value. The tone detected by the frequency detector (an earphone, for example) when the amplifier is in oscillation is readily distinguishable from the tone produced by the normal cell output signal thereby providing information for the operator as to whether or not operation is permissible.
An object of the present invention is to provide a simple, inexpensive temperature detection device.
Another object is to sense a predetermined temperature of an infra-red sensitive detection cell.
Still another object is to oscillate the amplifier of an infra-red sensitive detection cell when the temperature of the cell exceeds a predetermined value.
Still another object is to oscillate the amplifier of an infra-red sensitive detection cell by means of a regenerative feedback which is operative when the temperature of the cell exceeds a predetermined value.
3,089,034 Patented May 7, 1963 Still another object is to oscillate an amplifier by means of a regenerative feedback when the input voltage is at a predetermined value.
Other objects and many of the attendant advantages of this invention will become readily appreciated as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings wherein:
The FIGURE is a schematic diagram of the present invention.
In the drawing is shown detector cell 11 which is responsive to long wave length infra-red radiation. For successful operation, cells of this type must be maintained at very low temperatures, l96 C. for example, by means of separate refrigeration equipment shown by broken lines and designated generally by numeral 12. A detector cell of this type has a large negative temperature coelficient and when cooled to its operating temperature, 196 C. for example, its resistance will be approximately 3,500K ohms and when at room temperature its resistance will be approximately 50K ohms. The cell bias circuit consists of decoupling resistor 13 and cell load resistor 15 which series connect cell 11 with a B+ D.C. power supply. Capacitor 17 is provided to filter A.C. components from the DC. B+ power supply. It should be noted that the voltage at E between resistors 13 and 15, will decrease with increased detector cell temperature since the resistance of the detector cell decreases with increased temperature.
An R-C amplifier circuit is provided which is conventional and consists of triodes 21, '22 and 23 which are plate biased by B+ power through resistors 24, 25 and 26, respectively, and grid biased through resistors 27, 28 and 29, respectively. The output of cell 11 is coupled to the grid of triode 21 through coupling capacitor 31 and triodes 22 and 23 are coupled by capacitors 33 and 35, respectively. The triode 23 is of the cathode follower type, the cathode thereof being connected through resistor 37 to ground.
The feedback circuit is regenerative and connects the cathode of triode 23 to the grid of triode 2.1 through D.-C. blocking capacitor 38, diode 39, resistor 15 and capacitor 31. It can be seen that the feedback is regenerative since the phase shift from the grid of triode 21 to the grid of cathode follower triode 23 is 360 and since the cathode voltage follows the grid voltage of triode 23, the cathode of triode 23 has a 360' phase shift from the grid of triode 21. The cathode of diode 39 is biased by the voltage at B A voltage dividing network designated generally by numeral 41 provides a voltage E between resistors 42 and 43. The anode of diode 39 is biased by the voltage at E through current limiting resistor 44. Since very little current will flow through resistor 44, the potential at the cathode is virtually the same as the potential at E Diode 39, which may be of the silicon type, is used as a switch and provides infinite resistance when it is non-conducting. Diode 39 is non-conducting when E E and is conducting when E E The gain of the three stage amplifier is such that the amplifier will oscillate, at a frequency determined by the amplifier characteristics, when the regenerative feedback signal is applied to the input thereof. Voltage gain of the amplifier is sufiicient to cause oscillation even though the feedback is not connected directly to the grid but Reference Numeral Unit Value The operation of the device is as follows: When the cell is at its normal operating temperature (-196" C.) the voltage at E is approximately 155 volts. Since E is approximately 134 volts, diode 39 is reverse biased and provides infinite resistance. Therefore, the feedback from triode 23 is not applied to the grid of triode 21 and the amplifier functions as an amplifier of the signal from cell 11. As the temperature of cell 11 increases, the voltage at E decreases. Diode 39 will conduct when E decreases to a value less than E since it. is then forward biased. When diode 39 conducts, a regenerative feedback signal from the cathode of triode 2.3 is applied to the grid of triode 21 which causes the amplifier to oscillate at its natural frequency. The output of the amplifier is applied to a frequency responsive device, earphones for example, which indicates whether the amplifier is oscillating or is normally amplifying the cell output signal. "It can therefore be seen that when the cell becomes warm, the frequency responsive device indicates this condition (oscillation frequency) and the operator becomes aware that operation is not permissible. However, when the cell is cooled to its operation temperature, the operator is aware that operation is permissible.
Obviously many modifications and variations of the present invention are possible in the light of the above teachings. For example, different values of resistors, capacitors and biases could be selected, more or less amplifier stages could be employed so long as the regenerative feedback was of sufiicient strength to drive the amplifier into oscillation, diiferent amplifier designs could be employed, and the circuit could be employed to detect voltage characteristics other than those resulting from temperature changes. It is therefore to be understood that within the scope of the appended claims the invention may be practiced otherwise than as specifically described.
What is claimed is:
1. A detection device comprising an amplifier, a detection cell responsive to light energy, the resistance of said detection cell varying inversely with the temperature of said cell, a resistor, one side of said resistor being connected to a DC. potential source, the other side of said resistor being connected to one side of said detection cell, the other side of said detection cell being connected to ground, said one side of said detection cell being connected to the input of said amplifier, a regenerative feedback network for interconnecting the output and input of said amplifier, and means responsive to the voltage at said other side of said resistor for controlling transmission of the amplifier output signal through said network, wherein said last mentioned means comprises a diode the cathode of which is connected to said other side of said resistor and the anode of which is connected to a fixed D.C. potential, said diode being non-conducting when the voltage at said other side of said resistor is above a predetermined value, and transmitting said amplifier output signal when the voltage at said other side of said resistor is less than said predetermined value thereby causing oscillation of said amplifier 2. A detection device comprising an amplifier, a detection cell responsive to infra-red energy, the resistance of said detection cell varying inversely with the temperature of said cell, first and second resistors and said cell respectively connected in series with a DC. potential source, the input of said amplifier being connected between said second resistor and said cell, a regenerative feedback circuit comprising a diode, the cathode of said diode being connected between said first and second resistors and the anode of said diode being connected to the output of said amplifier and to a DC. potential source, the DC. voltage at said anode being less than the DC. voltage at said cathode when said cell is at a temperature not greater than a predetermined value, thereby preventing the transmission of the regenerative amplifier output signal to said input, and the DC. voltage at said anode being greater than the DJC. voltage at said cathode when the cell is at a temperature greater than said predetermined value, thereby permitting transmission of said regenerative output signal to said input and thereby causing said amplifier to oscillate.
3. The device of claim 2 wherein a frequency detection device is connected to the output of said amplifier for detecting whether the amplifier is oscillating.
References Cited in the file of this patent UNITED STATES PATENTS 1,542,937 Hammond June 23, 1925 2,419,052 Becker Apr. 15, 1947 2,473,197 Evans June 14, 1949 2,547,173 Rittner Apr. 3, 1951 2,616,020 Fay et al Oct. 28, 1952 2,816,233 Krueger Dec. 10, 1957 2,862,416 Doyle Dec. 2, 1958 2,870,310 Van Oberbeek Jan. 20, 1959 2,937,281 Bosch May 17, 1960 2,967,940 Erb et al. Jan. 10, 1961 2,984,729 Hykes et al May 16, 1961
Claims (1)
1. A DETECTION DEVICE COMPRISING AN AMPLIFIER, A DETECTION CELL RESPONSIVE TO LIGHT ENERGY, THE RESISTANCE OF SAID DETECTION CELL VARYING INVERSELY WITH THE TEMPERATURE OF SAID CELL, A RESISTOR, ONE SIDE OF SAID RESISTOR BEING CONNECTED TO A D.C. POTENTIAL SOURCE, THE OTHER SIDE OF SAID RESISTOR BEING CONNECTED TO ONE SIDE OF SAID DETECTION CELL, THE OTHER SIDE OF SAID DETECTION CELL BEING CONNECTED TO GROUND, SAID ONE SIDE OF SAID DETECTIOKN CELL BEING CONNECTED TO THE INPUT OF SAID AMPLIFIER, A REGENERATIVE FEEDBACK NETWORK FOR INTERCONNECTING THE OUTPUT AND INPUT OF SAID AMPLIFIER, AND MEANS RESPONSIVE TO THE VOLTAGE AT SAID OTHER SIDE OF SAID RESISTOR FOR CONROLLING TRANSMISSION OF THE AMPLIFIER OUTPUT SIGNAL THROUGH SAID NETWORK, WHEREIN SAID LAST MENTIONED MEANS COMPRISES A DIODE THE CATHODE OF WHICH IS CONNECTED TO SAID OTHER SIDE OF SSAID RESISTOR AND THE ANODE OF WHICH IS CONNECTED TO A FIXED D.C. POTENTIAL, SAID DIODE BEING NON-CONDUCTING WHEN THE VOLTAGE
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US53020A US3089034A (en) | 1960-08-30 | 1960-08-30 | Light sensitive detection circuit |
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US53020A US3089034A (en) | 1960-08-30 | 1960-08-30 | Light sensitive detection circuit |
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US53020A Expired - Lifetime US3089034A (en) | 1960-08-30 | 1960-08-30 | Light sensitive detection circuit |
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3335279A (en) * | 1964-06-24 | 1967-08-08 | Beckman Instruments Inc | Thermocouple radiation detector with an integrator in the feedback path of the amplifier to compensate for the integrating effect of the detector |
US3359425A (en) * | 1964-06-03 | 1967-12-19 | Harry M Smith | Sensory preception device |
US3363105A (en) * | 1963-02-28 | 1968-01-09 | Navy Usa | Temperature compensation of photoconductive detectors |
US3818230A (en) * | 1969-12-13 | 1974-06-18 | Tokyo Shibaura Electric Co | Bridge device for measuring the infrared radiation |
Citations (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US1542937A (en) * | 1920-05-08 | 1925-06-23 | Jr John Hays Hammond | Optical instrument |
US2419052A (en) * | 1943-09-30 | 1947-04-15 | Gen Electric | Thermionic energy detector |
US2473197A (en) * | 1945-06-21 | 1949-06-14 | Rca Corp | Heat detecting system |
US2547173A (en) * | 1950-03-09 | 1951-04-03 | Philips Lab Inc | Long wave length infrared radiation detector |
US2616020A (en) * | 1950-03-07 | 1952-10-28 | Shell Dev | Automatic temperature control |
US2816233A (en) * | 1954-01-28 | 1957-12-10 | Electronics Corp America | Ice detector |
US2862416A (en) * | 1954-06-09 | 1958-12-02 | Gen Electric | Light intensity measuring device including semiconductor translating circuit |
US2870310A (en) * | 1954-12-13 | 1959-01-20 | Philips Corp | Indicator circuit arrangement |
US2937281A (en) * | 1958-05-19 | 1960-05-17 | Sperry Rand Corp | Portable fm-ir detecting device |
US2967940A (en) * | 1959-03-05 | 1961-01-10 | Sperry Rand Corp | Transistorized fm-ir detector |
US2984729A (en) * | 1958-11-10 | 1961-05-16 | Collins Radio Co | Multivibrator type oven control |
-
1960
- 1960-08-30 US US53020A patent/US3089034A/en not_active Expired - Lifetime
Patent Citations (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US1542937A (en) * | 1920-05-08 | 1925-06-23 | Jr John Hays Hammond | Optical instrument |
US2419052A (en) * | 1943-09-30 | 1947-04-15 | Gen Electric | Thermionic energy detector |
US2473197A (en) * | 1945-06-21 | 1949-06-14 | Rca Corp | Heat detecting system |
US2616020A (en) * | 1950-03-07 | 1952-10-28 | Shell Dev | Automatic temperature control |
US2547173A (en) * | 1950-03-09 | 1951-04-03 | Philips Lab Inc | Long wave length infrared radiation detector |
US2816233A (en) * | 1954-01-28 | 1957-12-10 | Electronics Corp America | Ice detector |
US2862416A (en) * | 1954-06-09 | 1958-12-02 | Gen Electric | Light intensity measuring device including semiconductor translating circuit |
US2870310A (en) * | 1954-12-13 | 1959-01-20 | Philips Corp | Indicator circuit arrangement |
US2937281A (en) * | 1958-05-19 | 1960-05-17 | Sperry Rand Corp | Portable fm-ir detecting device |
US2984729A (en) * | 1958-11-10 | 1961-05-16 | Collins Radio Co | Multivibrator type oven control |
US2967940A (en) * | 1959-03-05 | 1961-01-10 | Sperry Rand Corp | Transistorized fm-ir detector |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3363105A (en) * | 1963-02-28 | 1968-01-09 | Navy Usa | Temperature compensation of photoconductive detectors |
US3359425A (en) * | 1964-06-03 | 1967-12-19 | Harry M Smith | Sensory preception device |
US3335279A (en) * | 1964-06-24 | 1967-08-08 | Beckman Instruments Inc | Thermocouple radiation detector with an integrator in the feedback path of the amplifier to compensate for the integrating effect of the detector |
US3818230A (en) * | 1969-12-13 | 1974-06-18 | Tokyo Shibaura Electric Co | Bridge device for measuring the infrared radiation |
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